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. 2018 May 21;4:7. doi: 10.1038/s41378-018-0008-3

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© The Author(s) 2018

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 3 — a Switching the chiral SPP modes. The as-deposited amorphous (AM) GST core is electrically heated beyond T_C = 433 K, allowing it to transform into crystalline (CR) GST under V_g = 17 V. V_g = 25 V is applied to heat the CR-GST beyond T_M = 873 K. Subsequent quenching leads to the melt-quenched (MQ) state GST. b Switching of the non-chiral SPP modes, where the AM-GST rod is electrically heated above T_C = 433 K by using V_g = 10 V